CA2216464A1 - Thermal processor for semiconductor wafers - Google Patents
Thermal processor for semiconductor wafers Download PDFInfo
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- CA2216464A1 CA2216464A1 CA002216464A CA2216464A CA2216464A1 CA 2216464 A1 CA2216464 A1 CA 2216464A1 CA 002216464 A CA002216464 A CA 002216464A CA 2216464 A CA2216464 A CA 2216464A CA 2216464 A1 CA2216464 A1 CA 2216464A1
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- reactor chamber
- coating
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- semiconductor wafer
- oxide
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Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 24
- 235000012431 wafers Nutrition 0.000 title description 31
- 238000000576 coating method Methods 0.000 claims abstract description 36
- 239000011248 coating agent Substances 0.000 claims abstract description 32
- 239000000463 material Substances 0.000 claims abstract description 19
- 230000005855 radiation Effects 0.000 claims abstract description 11
- 229910052736 halogen Inorganic materials 0.000 claims abstract description 8
- 150000002367 halogens Chemical class 0.000 claims abstract description 5
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 34
- 239000010453 quartz Substances 0.000 claims description 18
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 claims description 10
- 239000000377 silicon dioxide Substances 0.000 claims description 7
- SKRWFPLZQAAQSU-UHFFFAOYSA-N stibanylidynetin;hydrate Chemical compound O.[Sn].[Sb] SKRWFPLZQAAQSU-UHFFFAOYSA-N 0.000 claims description 6
- 229910052751 metal Inorganic materials 0.000 claims description 5
- 239000002184 metal Substances 0.000 claims description 5
- -1 indium-tin-oxide antimony-tin-oxide fluorine-tin-oxide Chemical compound 0.000 claims description 4
- 229910001507 metal halide Inorganic materials 0.000 claims description 4
- 150000005309 metal halides Chemical class 0.000 claims description 4
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 claims description 4
- 229910001887 tin oxide Inorganic materials 0.000 claims description 4
- NPNMHHNXCILFEF-UHFFFAOYSA-N [F].[Sn]=O Chemical compound [F].[Sn]=O NPNMHHNXCILFEF-UHFFFAOYSA-N 0.000 claims description 2
- AMGQUBHHOARCQH-UHFFFAOYSA-N indium;oxotin Chemical compound [In].[Sn]=O AMGQUBHHOARCQH-UHFFFAOYSA-N 0.000 claims description 2
- 150000004820 halides Chemical class 0.000 abstract 1
- 230000003340 mental effect Effects 0.000 abstract 1
- 235000012239 silicon dioxide Nutrition 0.000 description 13
- 238000000034 method Methods 0.000 description 12
- 230000008569 process Effects 0.000 description 11
- 238000010438 heat treatment Methods 0.000 description 10
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 9
- 229910052710 silicon Inorganic materials 0.000 description 9
- 239000010703 silicon Substances 0.000 description 9
- 229910052721 tungsten Inorganic materials 0.000 description 7
- 239000010937 tungsten Substances 0.000 description 7
- 238000010923 batch production Methods 0.000 description 4
- 239000007789 gas Substances 0.000 description 4
- WFKWXMTUELFFGS-UHFFFAOYSA-N tungsten Chemical compound [W] WFKWXMTUELFFGS-UHFFFAOYSA-N 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 3
- 238000002161 passivation Methods 0.000 description 3
- 229910052782 aluminium Inorganic materials 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
- 239000000969 carrier Substances 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 2
- 229910052753 mercury Inorganic materials 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 230000003647 oxidation Effects 0.000 description 2
- 238000007254 oxidation reaction Methods 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 229910052814 silicon oxide Inorganic materials 0.000 description 2
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 1
- 229910002601 GaN Inorganic materials 0.000 description 1
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- GWEVSGVZZGPLCZ-UHFFFAOYSA-N Titan oxide Chemical compound O=[Ti]=O GWEVSGVZZGPLCZ-UHFFFAOYSA-N 0.000 description 1
- 238000000862 absorption spectrum Methods 0.000 description 1
- 238000000429 assembly Methods 0.000 description 1
- 230000000712 assembly Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 238000005352 clarification Methods 0.000 description 1
- 230000001010 compromised effect Effects 0.000 description 1
- 239000000356 contaminant Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000000295 emission spectrum Methods 0.000 description 1
- 238000005265 energy consumption Methods 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 229910003437 indium oxide Inorganic materials 0.000 description 1
- PJXISJQVUVHSOJ-UHFFFAOYSA-N indium(iii) oxide Chemical compound [O-2].[O-2].[O-2].[In+3].[In+3] PJXISJQVUVHSOJ-UHFFFAOYSA-N 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- NJPPVKZQTLUDBO-UHFFFAOYSA-N novaluron Chemical compound C1=C(Cl)C(OC(F)(F)C(OC(F)(F)F)F)=CC=C1NC(=O)NC(=O)C1=C(F)C=CC=C1F NJPPVKZQTLUDBO-UHFFFAOYSA-N 0.000 description 1
- 230000008520 organization Effects 0.000 description 1
- BPUBBGLMJRNUCC-UHFFFAOYSA-N oxygen(2-);tantalum(5+) Chemical compound [O-2].[O-2].[O-2].[O-2].[O-2].[Ta+5].[Ta+5] BPUBBGLMJRNUCC-UHFFFAOYSA-N 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 229910010271 silicon carbide Inorganic materials 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 238000000391 spectroscopic ellipsometry Methods 0.000 description 1
- 229910001936 tantalum oxide Inorganic materials 0.000 description 1
- VXKWYPOMXBVZSJ-UHFFFAOYSA-N tetramethyltin Chemical compound C[Sn](C)(C)C VXKWYPOMXBVZSJ-UHFFFAOYSA-N 0.000 description 1
- OGIDPMRJRNCKJF-UHFFFAOYSA-N titanium oxide Inorganic materials [Ti]=O OGIDPMRJRNCKJF-UHFFFAOYSA-N 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
- PORFVJURJXKREL-UHFFFAOYSA-N trimethylstibine Chemical compound C[Sb](C)C PORFVJURJXKREL-UHFFFAOYSA-N 0.000 description 1
- 238000002211 ultraviolet spectrum Methods 0.000 description 1
- 238000001429 visible spectrum Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/26—Bombardment with radiation
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/67—Apparatus specially adapted for handling semiconductor or electric solid state devices during manufacture or treatment thereof; Apparatus specially adapted for handling wafers during manufacture or treatment of semiconductor or electric solid state devices or components ; Apparatus not specifically provided for elsewhere
- H01L21/67005—Apparatus not specifically provided for elsewhere
- H01L21/67011—Apparatus for manufacture or treatment
- H01L21/67098—Apparatus for thermal treatment
- H01L21/67115—Apparatus for thermal treatment mainly by radiation
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Toxicology (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Manufacturing & Machinery (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- High Energy & Nuclear Physics (AREA)
Abstract
A thermal processor for at least one semiconductor wafer includes a reactor chamber having a material substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers for holding the at least one semiconductor wafer. A coating including a material substantially reflective of infrared radiation can be present on at least a portion of the reactor chamber. A light source provides radiant energy to the at least one semiconductor wafer through the coating and the reactor chamber. The light source can include an ultraviolet discharge lamp, a halogen infrared incandescent lamp, or a mental halide visible discharge lamp. The coating can be situated on an inner or outer surface of the reactor chamber. If the reactor chamber has inner and outer walls, the coating can be situated on either the inner wall or the outer wall.
Description
CA 02216464 1997-09-2~
THERMAL PROCES~OR FOR
SEMICONDUCTOR WAFFRS
BACKGROUND OF THF INVF~TION
Silicon wafers have traditionally been processed in stages such as deposition, oxidation, and etching, for s example, in batches of twenty to forty wafers at a time.
The batches are processed inside quartz tubes wherein the wafers are held separately on quartz "wafer carriers". The tubes and wafers are heated by furnaces to a temperature ranging from about 800 ~C to about 1200 ~C. Typically 10 these furnaces are resistance heated furnace structures, such as furnaces heated with electric metal coils, and have processing times of several hours.
Single wafer processes have recently been developed.
Instead of long tubes with wafer carriers, smaller chambers 5 are used, and the time for processing one wafer can be on the order of one minute. One of the most prevalent single wafer processes uses a quartz chamber and is referred to as a rapid thermal process (RTP). RTP and other similar single wafer processes still heat the wafers from about 1000 ~C
20 to 1200 ~C; however, tungsten halogen lamps are used instead of resistive heating. Some batch processes likewise use tungsten halogen lamps instead of resistive heating. Such processes are generally referred to as ~fast batch processesU because they require more time than single 25 wafer ~rocesses but less time than traditional batch processes.
Conventional RTP systems for semiconductor manufacturing use the tungsten halogen lamps to rapidly - heat single silicon wafers laying horizontally within quartz 3 o parallel-plate reactors. In such systems, efficiency is compromised because the spectral emittance of tungsten CA 02216464 1997-09-2~
lamps is skewed toward the infrared region (where silicon absorption is low) and' because the heat irradiated by the hot silicon surfaces is transmitted through the reactor walls and lost outside the reactor. In addition to requiring 5 a large amount of electric power for the above reasons, heating variations' across the wafers are caused by the relative position of the wafers with respect to the lamps.
SUMMARY OF THF INVFI~ITION
It would be desirable to have a thermal processor for 10 semiconductor wafers with higher power efficiency (and correspondingly longer lamp life and lower energy consumption) than conventional processors.
It would also be desirable to have a thermal processor for semiconductor wafers with improved heating uniformity over conventional processors and there,by achieve a uniform surface temperature.
In one embodiment of the present invention, efficiency is increased by coating walls of a transparent reactor with a wavelength-selective layer to allow ultraviolet (UV) and visible radiation from the lamps to enter into the reactor while blocking the exit of infrared radiation emitted from the hot semiconductor wafers. Trapping the radiation within the reactor will increase the process efficiency by requiring less incident radiation onto the chamber and improve heating uniformity by increasing the fraction of indirect radiation that is insensitive to the lamp position.
In another embodiment, a halogen infrared incandescent lamp or a shorter wavelength mercury or metal halide discharge lamp is used which requires less 30 power than a tungsten lamp because it emits at a wavelength of higher silicon absorption. This lamp is also more reliable because a tungsten filament is not present.
CA 02216464 1997-09-2~
These two embodiments can be used individually or in combination in thermal processes such as single wafer processes, batch processes, rapid thermal processes, and fast batch processes, for example.
s BRIEF D~SCRIPTION OF THF DRAWINGS
The features of the invention believed to be novel are set forth with particularity in the appended claims. The invention itself, however, both as to organization and method of operation, together with further objects and 0 advantages thereof, may best be understood by reference to the following description taken in conjunction with the accompanying drawings, where like numerals represent like components, in which:
FIG, 1 is a sectional side view of a thermal processor 15 embodiment of t~e present invention.
FIG. 2 is a view similar to that of FIG. 1 wherein a wavelength selective coating is situated on an inner chamber wall and covered by a passivation layer.
FIG~. 3-5 are views similar to that of FIG. 1 with a 2 o double-wall chamber.
FIG. 6 is a sectional side view of a vertical thermal processor embodiment of the present invention.
D~TAI! Fn DF-~CRIPTION OF A
LI ~ LU FMBO~IMENT OF THE
INvFNTloN
FIG. 1 is a sectional side view of a thermal processor 25 embodiment 1 of the present invention. A semiconductor wafer 10 is positioned in a reactor chamber 12 and supported by small pins 14. The chamber has a wavelength selective coating 16 and receives radiant energy from lamp heating elements 18 and a lamp reflector 20.
CA 02216464 1997-09-2~
Wafer 10 may comprise any of a number of semiconductor materials such as silicon, silicon carbide, gallium arsenide, gallium nitride, for example. If desired, these semiconductor materials can be in combination with thin insulators and/or metal layers. Chamber 12 may comprise a material that is sufficiently optically transparent to permit high transmission of ultraviolet light and/or visible light (light including a wavelength within the range of about 200 nanometers to about 800 nanometers).
Examples of material for chamber 12 include quartz, quartz doped with alumina, alumina, and synthetic silica.
In the embodiment of FIG. 1, the wafer 10 is laid horizontally inside the chamber and is supported by pins 14 comprising quartz with the device surface facing the opposite side of the chamber (the non-pin side) and the lamp heating elements. The positioning of the wafer in the chamber is not critical. For example, the wafer can be supported in a slanted or vertical position or be supported by a quartz pedestal on the middle of the reactor chamber.
Coating 16 can be selected from any of a number of wavelength-selective materials that reflect infrared light such as, for example, indium-tin-oxide (ITO), antimony-tin-oxide (ATO), fluorine-tin-oxide (FTO), undoped tin oxide, dichroic filters, or thin metal films such as silver, aluminum, or gold. Dichroic filters may be fabricated of a stack of titanium oxide and silicon dioxide layers or tantalum oxide and silicon dioxide layers, for example, and are advantageous because they can survive for a long time at high temperatures. Like the chamber material, the 3 o coating material is capable of transmitting light including a wavelength within the range of about 200 nanometers to about 800 nanometers.
-CA 02216464 1997-09-2~
Infrared selective mirror coatings comprising doped semiconductor oxides, called Drude mirror coatings, have been characterized with regard to electrical, optical, and material properties as discussed in T. Gerfin and M. Gratzel, 5 "Optical properties of tin-doped indium oxide determined by spectroscopic ellipsometry", J. Appl. Phys., Vol. 79, pp.
1722-1729, 1 Feb. 1996. Drude mirror coatings have been used on glass panes of greenhouses to reduce energy losses caused by emission of infrared radiation while allowing 10 sunlight to enter freely as described in S.D. Silverstein, "Effect of Infrared Transparency on the Heat Transfer Through Windows: A Clarification of the Greenhouse Effect", Science, Vol. 193, pp. 229-31, 16 July 1976.
Antimony-tin-oxide (ATO) films have been deposited by 15 chemical vapor deposition on silicon oxide layers as described in T.P. Chow, M. Ghezzo, and B.J. Baliga, "Antimony-doped tin oxide films deposited by the oxidation of tetramethyltin and trimethylantimony", J. Electrochem.
Soc., pp. t040-45, May 1982, and it is therefore expected 20 that ATO films can be deposited on quartz. Dichroic filters have been used in halogen-lR parabolic aluminum reflector (PAR) lamps available from the General Electric Company, Cleveland, Ohio, to reflect infrared radiant heat from the iamp envelope while allowing the visible radiation to be 25 transmitted outside. The present invention differs from such halogen-lR. PAR lamps wherein the light source is inside the coated chamber bscause, in the present invention, the light source is situated outside the coated chamber.
Lamp heating elements 18 may comprise ultraviolet 30 (UV) discharge lamps such as mercury discharge lamps, metal halide visible discharge lamps, or halogen infrared incandescent lamps, for example. The wavelength range for the visible spectrum is from about 200 nanometers to about CA 02216464 1997-09-2~
400 nanometers, and the wavelength range for the UV
spectrum is from about 400 nanometers to about 800 nanometers. Therefore, chamber 12 and coating 16 are preferably capable of passing light at a wavelength included s in a range of about 200 nanometers to about 800 nanometers.
If the lamp heating elements are cylindrical, they can be lined up in parallel at a periodic distance from each other and at an equal distance from the semiconductor wafer.
10 Lamp reflector 20 may comprise a group of concave mirrors 22 placed above the lamps to efficiently reflect the back illumination of the lamps.
Using a UV discharge lamp to process silicon wafers, for example, is expected to increase the light utilization 15 efficiently by thirty percent or more over conventional tungsten lamp designs even without a coating on the chamber. The expected increase in efficiency is due to the fact that the silicon absorption spectrum has a larger overlap with the emission spectrum of the discharge lamp.
20 Using the coating to provide heat recovery is expected to improve power efficiency by about an additional sixty-five percent. An-overall improvement of about ninety-five percent is expected.
FIG. 2 is a view similar to that of FIG. 1 wherein a 25 wavelength selective coating 16a is situated on the inner side of chamber wall 12a and covered by a passivation layer 24. Situating the coating on a wall inner side helps to reduce absorption of the IR radiation by the chamber wall 12a. The coating in this embodiment should be a refractory 30 material that does not shed any particles onto the wafer and is free of contaminants. Passivation layer 24 may comprise a material such as, for example, silicon oxide (siO2) having a thickness in the range of about 0.1 microns to about 0.2 CA 02216464 1997-09-2~
microns and can be added to coating 16a of FIG. 2 or coating 16 of FIG. 1 to protect the coating.
FlGs. 3-5 are views similar to that of FIG. 1 with a double-wall chamber for gas cooling which is useful if a single wall would result in the chamber wall temperature exceeding the thermal capability of the coating. This is useful because silicon wafers, for example, can reach temperatures exceeding 1000 ~C. In FlGs. 3 and 4, the coatings 16b and 16c, respectively, are positioned between 10 chamber walls 12b and 26, and 12c and 26c, respectively.
Forced air 28 and 28c can be pumped between chamber walls. In FIG. 3, coating 16b is situated on an outer surface of chamber wall 12b, and in FIG. 4, coating 16c is situated on an inner surface of chamber wall 28c. In FIG. 5, chamber 15 walls 12d and 26d have forced air 28d pumped therebetween and coating 16d is present on an inner surface of chamber wall 12d. Furthermore, FIG. 5 illustrates a plurality of wafers 10a and 10b in a single chamber 12d.
FIG. 6 is a sectional side view of a vertical thermal 20 processor embodiment 2 of the present invention wherein chamber 612 is coated with wavelength selective coating 616 and encloses a plurality of wafers 610 which can be stacked using quartz pins (not shown), for example. The chamber is sealed by cap 630 which may comprise a 2~ material such as quartz, for example. Gases such as N2, ~2.
or pyrogenic-generated steam can be supplied through gas inlet port 632 and released through gas outlet port 634.
Radiant energy is supplied by lamp heating elements 618 of lamp assemblies 619.
While only certain preferred features of the invention have been illustrated and described herein, many modifications and changes will occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all such modifications and changes as fall within the true spirit of the invention.
THERMAL PROCES~OR FOR
SEMICONDUCTOR WAFFRS
BACKGROUND OF THF INVF~TION
Silicon wafers have traditionally been processed in stages such as deposition, oxidation, and etching, for s example, in batches of twenty to forty wafers at a time.
The batches are processed inside quartz tubes wherein the wafers are held separately on quartz "wafer carriers". The tubes and wafers are heated by furnaces to a temperature ranging from about 800 ~C to about 1200 ~C. Typically 10 these furnaces are resistance heated furnace structures, such as furnaces heated with electric metal coils, and have processing times of several hours.
Single wafer processes have recently been developed.
Instead of long tubes with wafer carriers, smaller chambers 5 are used, and the time for processing one wafer can be on the order of one minute. One of the most prevalent single wafer processes uses a quartz chamber and is referred to as a rapid thermal process (RTP). RTP and other similar single wafer processes still heat the wafers from about 1000 ~C
20 to 1200 ~C; however, tungsten halogen lamps are used instead of resistive heating. Some batch processes likewise use tungsten halogen lamps instead of resistive heating. Such processes are generally referred to as ~fast batch processesU because they require more time than single 25 wafer ~rocesses but less time than traditional batch processes.
Conventional RTP systems for semiconductor manufacturing use the tungsten halogen lamps to rapidly - heat single silicon wafers laying horizontally within quartz 3 o parallel-plate reactors. In such systems, efficiency is compromised because the spectral emittance of tungsten CA 02216464 1997-09-2~
lamps is skewed toward the infrared region (where silicon absorption is low) and' because the heat irradiated by the hot silicon surfaces is transmitted through the reactor walls and lost outside the reactor. In addition to requiring 5 a large amount of electric power for the above reasons, heating variations' across the wafers are caused by the relative position of the wafers with respect to the lamps.
SUMMARY OF THF INVFI~ITION
It would be desirable to have a thermal processor for 10 semiconductor wafers with higher power efficiency (and correspondingly longer lamp life and lower energy consumption) than conventional processors.
It would also be desirable to have a thermal processor for semiconductor wafers with improved heating uniformity over conventional processors and there,by achieve a uniform surface temperature.
In one embodiment of the present invention, efficiency is increased by coating walls of a transparent reactor with a wavelength-selective layer to allow ultraviolet (UV) and visible radiation from the lamps to enter into the reactor while blocking the exit of infrared radiation emitted from the hot semiconductor wafers. Trapping the radiation within the reactor will increase the process efficiency by requiring less incident radiation onto the chamber and improve heating uniformity by increasing the fraction of indirect radiation that is insensitive to the lamp position.
In another embodiment, a halogen infrared incandescent lamp or a shorter wavelength mercury or metal halide discharge lamp is used which requires less 30 power than a tungsten lamp because it emits at a wavelength of higher silicon absorption. This lamp is also more reliable because a tungsten filament is not present.
CA 02216464 1997-09-2~
These two embodiments can be used individually or in combination in thermal processes such as single wafer processes, batch processes, rapid thermal processes, and fast batch processes, for example.
s BRIEF D~SCRIPTION OF THF DRAWINGS
The features of the invention believed to be novel are set forth with particularity in the appended claims. The invention itself, however, both as to organization and method of operation, together with further objects and 0 advantages thereof, may best be understood by reference to the following description taken in conjunction with the accompanying drawings, where like numerals represent like components, in which:
FIG, 1 is a sectional side view of a thermal processor 15 embodiment of t~e present invention.
FIG. 2 is a view similar to that of FIG. 1 wherein a wavelength selective coating is situated on an inner chamber wall and covered by a passivation layer.
FIG~. 3-5 are views similar to that of FIG. 1 with a 2 o double-wall chamber.
FIG. 6 is a sectional side view of a vertical thermal processor embodiment of the present invention.
D~TAI! Fn DF-~CRIPTION OF A
LI ~ LU FMBO~IMENT OF THE
INvFNTloN
FIG. 1 is a sectional side view of a thermal processor 25 embodiment 1 of the present invention. A semiconductor wafer 10 is positioned in a reactor chamber 12 and supported by small pins 14. The chamber has a wavelength selective coating 16 and receives radiant energy from lamp heating elements 18 and a lamp reflector 20.
CA 02216464 1997-09-2~
Wafer 10 may comprise any of a number of semiconductor materials such as silicon, silicon carbide, gallium arsenide, gallium nitride, for example. If desired, these semiconductor materials can be in combination with thin insulators and/or metal layers. Chamber 12 may comprise a material that is sufficiently optically transparent to permit high transmission of ultraviolet light and/or visible light (light including a wavelength within the range of about 200 nanometers to about 800 nanometers).
Examples of material for chamber 12 include quartz, quartz doped with alumina, alumina, and synthetic silica.
In the embodiment of FIG. 1, the wafer 10 is laid horizontally inside the chamber and is supported by pins 14 comprising quartz with the device surface facing the opposite side of the chamber (the non-pin side) and the lamp heating elements. The positioning of the wafer in the chamber is not critical. For example, the wafer can be supported in a slanted or vertical position or be supported by a quartz pedestal on the middle of the reactor chamber.
Coating 16 can be selected from any of a number of wavelength-selective materials that reflect infrared light such as, for example, indium-tin-oxide (ITO), antimony-tin-oxide (ATO), fluorine-tin-oxide (FTO), undoped tin oxide, dichroic filters, or thin metal films such as silver, aluminum, or gold. Dichroic filters may be fabricated of a stack of titanium oxide and silicon dioxide layers or tantalum oxide and silicon dioxide layers, for example, and are advantageous because they can survive for a long time at high temperatures. Like the chamber material, the 3 o coating material is capable of transmitting light including a wavelength within the range of about 200 nanometers to about 800 nanometers.
-CA 02216464 1997-09-2~
Infrared selective mirror coatings comprising doped semiconductor oxides, called Drude mirror coatings, have been characterized with regard to electrical, optical, and material properties as discussed in T. Gerfin and M. Gratzel, 5 "Optical properties of tin-doped indium oxide determined by spectroscopic ellipsometry", J. Appl. Phys., Vol. 79, pp.
1722-1729, 1 Feb. 1996. Drude mirror coatings have been used on glass panes of greenhouses to reduce energy losses caused by emission of infrared radiation while allowing 10 sunlight to enter freely as described in S.D. Silverstein, "Effect of Infrared Transparency on the Heat Transfer Through Windows: A Clarification of the Greenhouse Effect", Science, Vol. 193, pp. 229-31, 16 July 1976.
Antimony-tin-oxide (ATO) films have been deposited by 15 chemical vapor deposition on silicon oxide layers as described in T.P. Chow, M. Ghezzo, and B.J. Baliga, "Antimony-doped tin oxide films deposited by the oxidation of tetramethyltin and trimethylantimony", J. Electrochem.
Soc., pp. t040-45, May 1982, and it is therefore expected 20 that ATO films can be deposited on quartz. Dichroic filters have been used in halogen-lR parabolic aluminum reflector (PAR) lamps available from the General Electric Company, Cleveland, Ohio, to reflect infrared radiant heat from the iamp envelope while allowing the visible radiation to be 25 transmitted outside. The present invention differs from such halogen-lR. PAR lamps wherein the light source is inside the coated chamber bscause, in the present invention, the light source is situated outside the coated chamber.
Lamp heating elements 18 may comprise ultraviolet 30 (UV) discharge lamps such as mercury discharge lamps, metal halide visible discharge lamps, or halogen infrared incandescent lamps, for example. The wavelength range for the visible spectrum is from about 200 nanometers to about CA 02216464 1997-09-2~
400 nanometers, and the wavelength range for the UV
spectrum is from about 400 nanometers to about 800 nanometers. Therefore, chamber 12 and coating 16 are preferably capable of passing light at a wavelength included s in a range of about 200 nanometers to about 800 nanometers.
If the lamp heating elements are cylindrical, they can be lined up in parallel at a periodic distance from each other and at an equal distance from the semiconductor wafer.
10 Lamp reflector 20 may comprise a group of concave mirrors 22 placed above the lamps to efficiently reflect the back illumination of the lamps.
Using a UV discharge lamp to process silicon wafers, for example, is expected to increase the light utilization 15 efficiently by thirty percent or more over conventional tungsten lamp designs even without a coating on the chamber. The expected increase in efficiency is due to the fact that the silicon absorption spectrum has a larger overlap with the emission spectrum of the discharge lamp.
20 Using the coating to provide heat recovery is expected to improve power efficiency by about an additional sixty-five percent. An-overall improvement of about ninety-five percent is expected.
FIG. 2 is a view similar to that of FIG. 1 wherein a 25 wavelength selective coating 16a is situated on the inner side of chamber wall 12a and covered by a passivation layer 24. Situating the coating on a wall inner side helps to reduce absorption of the IR radiation by the chamber wall 12a. The coating in this embodiment should be a refractory 30 material that does not shed any particles onto the wafer and is free of contaminants. Passivation layer 24 may comprise a material such as, for example, silicon oxide (siO2) having a thickness in the range of about 0.1 microns to about 0.2 CA 02216464 1997-09-2~
microns and can be added to coating 16a of FIG. 2 or coating 16 of FIG. 1 to protect the coating.
FlGs. 3-5 are views similar to that of FIG. 1 with a double-wall chamber for gas cooling which is useful if a single wall would result in the chamber wall temperature exceeding the thermal capability of the coating. This is useful because silicon wafers, for example, can reach temperatures exceeding 1000 ~C. In FlGs. 3 and 4, the coatings 16b and 16c, respectively, are positioned between 10 chamber walls 12b and 26, and 12c and 26c, respectively.
Forced air 28 and 28c can be pumped between chamber walls. In FIG. 3, coating 16b is situated on an outer surface of chamber wall 12b, and in FIG. 4, coating 16c is situated on an inner surface of chamber wall 28c. In FIG. 5, chamber 15 walls 12d and 26d have forced air 28d pumped therebetween and coating 16d is present on an inner surface of chamber wall 12d. Furthermore, FIG. 5 illustrates a plurality of wafers 10a and 10b in a single chamber 12d.
FIG. 6 is a sectional side view of a vertical thermal 20 processor embodiment 2 of the present invention wherein chamber 612 is coated with wavelength selective coating 616 and encloses a plurality of wafers 610 which can be stacked using quartz pins (not shown), for example. The chamber is sealed by cap 630 which may comprise a 2~ material such as quartz, for example. Gases such as N2, ~2.
or pyrogenic-generated steam can be supplied through gas inlet port 632 and released through gas outlet port 634.
Radiant energy is supplied by lamp heating elements 618 of lamp assemblies 619.
While only certain preferred features of the invention have been illustrated and described herein, many modifications and changes will occur to those skilled in the art. It is, therefore, to be understood that the appended claims are intended to cover all such modifications and changes as fall within the true spirit of the invention.
Claims (10)
1. A thermal processor for at least one semiconductor wafer comprising:
a reactor chamber for holding the at least one semiconductor wafer the reactor chamber comprising a material substantially transparent to light including a wavelength, within a range of about 200 nanometers to about 800 nanometer;
a coating on at least a portion of the reactor chamber, the coating comprising materials substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers and substantially reflective of infrared radiation; and a light source for providing radiant energy to the at least one semiconductor wafer through the coating and the reactor chamber.
a reactor chamber for holding the at least one semiconductor wafer the reactor chamber comprising a material substantially transparent to light including a wavelength, within a range of about 200 nanometers to about 800 nanometer;
a coating on at least a portion of the reactor chamber, the coating comprising materials substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers and substantially reflective of infrared radiation; and a light source for providing radiant energy to the at least one semiconductor wafer through the coating and the reactor chamber.
2. The processor of claim 1 wherein the light source is an ultraviolet discharge lamp a halogen infrared incandescent lamp or a 15 metal halide visible discharge lamp.
3. The processor of claim 1 wherein the reactor chamber is quartz alumina doped quartz alumina or synthetic silica.
4. The processor of claim 1 wherein the coating is indium-tin-oxide antimony-tin-oxide fluorine-tin-oxide undoped tin oxide a dichroic filter or a thin metal film.
5. A thermal processor for at least one semiconductor wafer comprising:
a reactor chamber for holding the at least one semiconductor wafer the reactor chamber comprising a material substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers; and a lamp comprising an ultraviolet discharge lamp, a halogen infrared incandescent lamp, or a metal halide visible discharge lamp, the lamp capable of providing radiant energy to the at least one semiconductor wafer through the reactor chamber.
a reactor chamber for holding the at least one semiconductor wafer the reactor chamber comprising a material substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers; and a lamp comprising an ultraviolet discharge lamp, a halogen infrared incandescent lamp, or a metal halide visible discharge lamp, the lamp capable of providing radiant energy to the at least one semiconductor wafer through the reactor chamber.
6. The processor of claim 5, wherein the reactor chamber is quartz, alumina doped quartz, alumina, or synthetic silica.
7. A thermal processor for at least one semiconductor wafer comprising:
a substantially transparent reactor chamber for holding the at least one semiconductor wafer;
a coating comprising a selective infrared reflective material covering at least a portion of the reactor chamber, and an ultraviolet discharge lamp for providing radiant energy to the at least one semiconductor wafer through the coating and the reactor chamber.
a substantially transparent reactor chamber for holding the at least one semiconductor wafer;
a coating comprising a selective infrared reflective material covering at least a portion of the reactor chamber, and an ultraviolet discharge lamp for providing radiant energy to the at least one semiconductor wafer through the coating and the reactor chamber.
8. The processor of claim 7, wherein the reactor chamber is quartz, alumina doped quartz, alumina, or synthetic silica and the coating is indium-tin-oxide, antimony-tin-oxide, fluorine-tin-oxide, undoped tin oxide, a dichroic filter or a thin metal film.
9. An apparatus for use in a thermal processor, the apparatus comprising:
a reactor chamber for holding at least one semiconductor wafer, the reactor chamber comprising a material substantially transparent to light including a wavelength within a range of about 200 nanometers to about 800 nanometers; and a coating on at least a portion of the reactor chamber, the coating comprising material substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers and substantially reflective of infrared radiation.
a reactor chamber for holding at least one semiconductor wafer, the reactor chamber comprising a material substantially transparent to light including a wavelength within a range of about 200 nanometers to about 800 nanometers; and a coating on at least a portion of the reactor chamber, the coating comprising material substantially transparent to light including a wavelength within the range of about 200 nanometers to about 800 nanometers and substantially reflective of infrared radiation.
10. The apparatus of claim 9, wherein the reactor chamber is quartz, alumina doped quark, alumina, or synthetic silica.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US08/743,587 US6067931A (en) | 1996-11-04 | 1996-11-04 | Thermal processor for semiconductor wafers |
US08/743,587 | 1996-11-04 |
Publications (1)
Publication Number | Publication Date |
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CA2216464A1 true CA2216464A1 (en) | 1998-05-04 |
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ID=24989354
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CA002216464A Abandoned CA2216464A1 (en) | 1996-11-04 | 1997-09-25 | Thermal processor for semiconductor wafers |
Country Status (9)
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US (1) | US6067931A (en) |
EP (1) | EP0840359A3 (en) |
JP (1) | JPH10256171A (en) |
KR (1) | KR19980041866A (en) |
CA (1) | CA2216464A1 (en) |
IL (1) | IL122034A (en) |
RU (1) | RU2185682C2 (en) |
SG (1) | SG55398A1 (en) |
TW (1) | TW457594B (en) |
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-
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- 1996-11-04 US US08/743,587 patent/US6067931A/en not_active Expired - Fee Related
-
1997
- 1997-08-30 KR KR1019970045103A patent/KR19980041866A/en not_active Application Discontinuation
- 1997-09-25 CA CA002216464A patent/CA2216464A1/en not_active Abandoned
- 1997-10-03 TW TW086114413A patent/TW457594B/en not_active IP Right Cessation
- 1997-10-23 SG SG1997003852A patent/SG55398A1/en unknown
- 1997-10-27 IL IL12203497A patent/IL122034A/en not_active IP Right Cessation
- 1997-10-30 JP JP9297616A patent/JPH10256171A/en not_active Withdrawn
- 1997-11-03 RU RU97118326/28A patent/RU2185682C2/en not_active IP Right Cessation
- 1997-11-04 EP EP97308821A patent/EP0840359A3/en not_active Withdrawn
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KR19980041866A (en) | 1998-08-17 |
EP0840359A3 (en) | 2002-04-03 |
TW457594B (en) | 2001-10-01 |
SG55398A1 (en) | 1998-12-21 |
IL122034A (en) | 2001-05-20 |
JPH10256171A (en) | 1998-09-25 |
MX9708509A (en) | 1998-05-31 |
RU2185682C2 (en) | 2002-07-20 |
US6067931A (en) | 2000-05-30 |
EP0840359A2 (en) | 1998-05-06 |
IL122034A0 (en) | 1998-03-10 |
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FZDE | Discontinued |